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Self-focusing and Wakefield-focusing of Relativistic Electron Bunches in Plasma
It was shown that at the wakefield excitation by electron bunch, the length of which is equal to half of the wavelength, the ratio of wakefield focusing to self-focusing is large at the end of the bunch, the shape of which is such that it falls from the current maximum value in the head of the bunch to zero at the end of the bunch. However, the ratio of wakefield focusing to self-focusing tends to zero at the end of the bunch, if the current increases along the bunch from zero in the head ofdoi:10.18429/jacow-ipac2016-wepmy023 fatcat:nofdg2ajrjg23djtr55kpj2xgy